The photon energy distributions of the first three resonance lines of heliumlike argon broadened by the local fields of both ions and electrons are calculated for dense H, D, or T plasmas containing small amounts of argon. The electron collisions are treated by an impact theory allowing for both widths and shifts in the distorted-wave approximation to all significant orders of the multipole expansion for the electron-radiator interaction. Ion effects are treated in the quasistatic approximation for dipole interactions between ions and radiators. These interactions between states of a given principal quantum number are calculated in the intermediate-coupling representation, using ion-field-strength distribution functions calculated by Boercker with the method of Iglesias et al [Phys. Rev. A 28, 1667 (1983)]. The profiles obtained were corrected for thermal Doppler broadening and also for ion-dynamical effects according to Stamm et al. [Phys. Rev. A 34, 4144 (1986)].
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